Structural color from a coupled nanowire pair beyond the bonding and antibonding model
Optical resonances in nanostructures can be harnessed to produce a wide range of structural colors. Conversely, the analysis of structural colors has been used to clarify the nature of optical resonances. Here, we show that silicon nanowire (NW) pairs can display a wide range of structural colors by...
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Published in | Optica Vol. 8; no. 4; p. 464 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
Published |
United States
Optical Society of America - OSA Publishing
01.04.2021
Optical Society of America |
Subjects | |
Online Access | Get full text |
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Summary: | Optical resonances in nanostructures can be harnessed to produce a wide range of structural colors. Conversely, the analysis of structural colors has been used to clarify the nature of optical resonances. Here, we show that silicon nanowire (NW) pairs can display a wide range of structural colors by controlling their radiative coupling. This is accomplished by exciting a series of Fabry–Pérot-like modes where light is repeatedly scattered between two NWs. These modes are beyond the expectation from the conventional chemical bonding model under a quasi-electrostatic approximation, in which only bonding and antibonding modes can be formed in a pair system through modal hybridization. The additional eigenmodes found in a two-resonator system originate from the nonlinear, frequency-dependent coupling strength derived from the radiative nature of low- Q resonators. The Fabry–Pérot modes can be tuned across the entire visible frequency range by varying the distance between two NWs, leading to what we believe is a new type of universal building blocks that can provide structural color within a subwavelength footprint. The presented results pave the way toward the design and usage of highly tunable resonances that exploit the radiative coupling of high-index nanostructures. |
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Bibliography: | FG07-ER46426 USDOE |
ISSN: | 2334-2536 2334-2536 |
DOI: | 10.1364/OPTICA.418888 |